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    4.

    The dimensional formula of coefficient of permittivity for free space (ε0)\left( {{\varepsilon _0}} \right) in the equation F=14πε0q1q2r2,F = \frac{1}{{4{\rm{\pi }}{\varepsilon _0}}}\frac{{{q_1}{q_2}}}{{{r^2}}}, where symbols have their usual meanings, is

    A

    [ML3A2T4]\left[ {{\rm{M}}{{\rm{L}}^3}{{\rm{A}}^{ - 2}}{{\rm{T}}^{ - 4}}} \right]

    B

    [M1L3T4A2]\left[ {{{\rm{M}}^{ - 1}}{{\rm{L}}^{ - 3}}{{\rm{T}}^4}{{\rm{A}}^2}} \right]

    C

    [M1L3A2T4]\left[ {{{\rm{M}}^{ - 1}}{{\rm{L}}^{ - 3}}{{\rm{A}}^{ - 2}}{{\rm{T}}^{ - 4}}} \right]

    D

    [ML3A2T4]\left[ {{\rm{M}}{{\rm{L}}^3}{{\rm{A}}^2}{{\rm{T}}^{ - 4}}} \right]

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    8.

    The velocity v of water waves may depend on their wavelength (λ\lambda ), the density of water (ρ\rho ) and the acceleration due to gravity (g). The method of dimensions gives the relation between these quantities as

    A

    v2λ1ρ1{v^2} \propto {\lambda ^{ - 1}}{\rho ^{ - 1}}

    B

    v2gλ{v^2} \propto {\rm{g}}\lambda

    C

    v2gλρ{v^2} \propto {\rm{g}}\lambda \rho

    D

    g1λ3{{\rm{g}}^{ - 1}} \propto {\lambda ^3}

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